The sensory epithelium of the bullfrog's sacculus can be employed in various configurations to probe the physiology of hair cells. Because the tissue is relatively flat, it can be mounted in both one- and two-chamber preparations. The one-chamber configuration provides a simple setup for electrophysiological and micromechanical recordings of hair cells. The two-chamber preparation instead simulates both the endolymphatic and perilymphatic compartments on respectively the apical and basal sides of hair cells. These compartments together provide a physiologically-relevant environment for the study of mechanotransduction by hair cells.
The sensitivity and transduction characteristics of hair cells underlie their electrical response to mechanical stimulation. To probe these features, we simultaneously recorded from an individual hair cell the position of its bundle and the cell's receptor potential (Figure 2). We first attached a flexible glass fiber to the kinociliary bulb of a hair bundle to apply force pulses. We then measured the hair bundle's displacement using a dual photodiode system2 (Figure 2A). We concurrently acquired the hair cell's potential by impaling the cell with a sharp microelectrode. We obtained a displacement-response curve by plotting the peak voltage response elicited by each mechanical stimulus against the hair bundle's corresponding displacement (Figure 2B). The hair cell's electrical response saturates for both positive- and negative-displacement extrema. The reduction of membrane potential with negative displacement steps indicates the presence of a resting inward mechanotransduction current. This resting current is modulated by the action of Ca2+ on both fast and slow adaptation17,18,19,20,21.
A hair cell's behavior depends not only upon its electrical properties, but also upon the micromechanics of its sensory hair bundle. The two-chamber configuration mimics the separation of endolymph and perilymph in vivo, providing ideal conditions for the study of a hair bundle's mechanics. Under these conditions and with the otolithic membrane removed, hair bundles can oscillate spontaneously6. Here we employed the two-chamber preparation to assess the micromechanics of individual bundles. We recorded the spontaneous oscillations of a hair bundle by casting its shadow on a dual-photodiode displacement monitor (Figure 3). To assess the role of the aminoglycoside antibiotic gentamicin on mechanotransduction, we iontophoretically released gentamicin directly onto the hair bundle (Figure 3). The concentration of released gentamicin rises proportionally with the current passed through the micropipette. Gentamicin inhibits a hair bundle's oscillations and induces a static offset of the bundle towards its tall side. These effects reflect the role of gentamicin as an open-channel blocker that maintains the open state of mechanotransduction channels while blocking their permeation pore. Iontophoresis of charged chemicals permits localized and quantifiable release of chemicals at various concentrations in the absence of fluid flow-induced mechanical disruption and is thus ideally suited for the study of mechanosensitive organelles such as the hair bundle22.
A hair bundle's spontaneous motion arises from the interplay between adaptation and nonlinear bundle stiffness7,8,23,24. This spontaneous motion is a signature of a hair bundle's active process, which converts signal energy into mechanical work to overcome viscous drag. Hair bundles have been shown to exhibit nonlinear instantaneous stiffness in the vestibular2, auditory25, and lateral-line systems26.
We directly measured the instantaneous stiffness of an individual hair bundle from the bullfrog's sacculus (Figure 4). To achieve this, we coupled the tip of a flexible glass fiber to the hair bundle's kinociliary bulb (Figure 4A). We delivered forces to the hair bundle by displacing the fiber's base. The force exerted onto the hair bundle by the stimulus fiber corresponds to the difference between the displacements of the fiber's base and tip, multiplied by the fiber's stiffness2,27. Delivering pulses across a range of forces reveals a relationship between the force exerted onto the bundle and the bundle's ensuing displacement. The slope of this force-displacement relation corresponds to the hair bundle's instantaneous stiffness (Figure 4A).
This method allowed us to measure an individual bundle's instantaneous stiffness as a function of its deflection (Figure 4B). The instantaneous force-displacement curve displays a nonlinear relationship, revealing a nonlinear stiffness of the bundle over a range of about 20 nm around its resting position. Outside this range, the hair bundle behaves like a Hookean material, its stiffness is linear for large-magnitude deflections.
These results demonstrate the versatility of the bullfrog sacculus in the study of hair-cell physiology. Using these and other preparations, one can explore mechanotransduction at multiple stages in the transmission of information from the bundle toward the brain.

Figure 1: Dissection of the Bullfrog's Inner Ear. (A) Viewing the bullfrog's upper palate from its ventral side permits identification of the Eustachian tube (circle). Lateral reflection of the skin covering the right side of the upper palate reveals the location of the inner ear (dashed box). (B) Removal of the cartilage on the ventral side of the frog's temporal bone opens the otic capsule (dashed line). (C) Displayed is a higher magnification image of the otic capsule, in which the sacculus, lagena, CN VIII, and saccular nerve can be readily identified. (D) A view of the otic capsule after removal of the inner-ear organs reveals the locations of the semicircular canals. (E) After removal of the isolated inner ear, the sacculus, lagena, and VIIIth cranial nerve (CN VIII) can readily be identified. (F) The isolated sacculus possesses a short stump of the saccular nerve and an otolithic membrane lying atop its sensory epithelium. Labels correspond to the (i) sacculus, (ii) lagena, (iii) CN VIII, (iv) saccular nerve, and (v) otolithic membrane. Axis labels P and A correspond respectively to the posterior and anterior directions. Scale bars represent 1 cm (A, B), 1 mm (C, D, E), and 400 μm (F).
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Figure 2: Displacement-response Curve for a Single Hair Cell. (A) The tip of a glass stimulus fiber was coupled to the kinociliary bulb of a hair bundle and the fiber's base was subsequently displaced across nine discrete steps. The bundle's position was tracked on a dual-photodiode system, and its receptor potential was simultaneously measured using a microelectrode whose output was passed through an amplifier in bridge mode. The electrode's tip resistance was 95 MΩ and the bundle's resting membrane potential was -47 mV. (B) A plot of the bundle's receptor potential as a function of its displacement reveals a nonlinear relationship between the bundle's response and its position. Each point corresponds to the mean potential and mean displacement over a 2.5 ms time window, beginning 2.5 ms after the onset of mechanical stimulation. Each color represents a set of time series corresponding to the same displacement pulse.
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Figure 3: Effect of Gentamicin on Spontaneous Hair Bundle Oscillation. The spontaneous motion of a hair bundle in a two-chamber preparation was recorded using a dual photodiode system. In the absence of iontophoretic release of gentamicin (0 nA), the hair bundle displays symmetric oscillations. As the magnitude of current passed through an iontophoretic pipette filled with 500 mM gentamicin sulfate grows (10 nA, 20 nA), the frequency of hair-bundle excursions falls in a dose-dependent manner and the bundle is offset towards its tall edge for longer periods of time.
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Figure 4. Calculating a Hair Bundle's Instantaneous Stiffness. (A) A stimulus fiber (red) of stiffness KF is coupled to the kinociliary bulb (brown) of an individual hair bundle (yellow). Displacing the base of the fiber a known distance XF causes the bundle to move a distance XB. The difference between the displacements of the fiber and the bundle is proportional to the force exerted onto the bundle by the stimulus fiber, FF. Repeating this across a range of forces yields an instantaneous force-displacement relation (right), the slope of which corresponds to the hair bundle's instantaneous stiffness. (B) An individual bundle was subjected to force pulses of increasing magnitude and its displacement within the first 50 ms after the pulse onset was measured (blue points). Here the hair bundle displays a nonlinear instantaneous stiffness over a range of approximately 20 nm around its resting position. The red curve corresponds to a fit to the relation F = k*X - 60*z*(1/(1+exp(-z*(X-X0)/(kB*T))) + F0, in which F is the force applied to the bundle, X is the bundle's displacement, k = 790 ± 51 µN∙m-1 is the bundle's constant stiffness when all channels are either closed or open, z = 0.43 ± 0.04 pN is the force of a single gating spring, X0 = 2 ± 1.9 nm is the bundle's position at which 50% of its channels are open, kB is Boltzmann's constant, T is the temperature, and F0 = 11.7 ± 1.3 pN is an offset force. The fit possesses a coefficient of determination of 0.98. The stimulus fiber had a stiffness of 107 µN∙m-1.
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| Solute | Formula Weight (g/mol) | Add to 1 L |
| Artificial perilymph | Artificial endolymph |
| NaCl | 58.4 | 6.54 g | 0.117 g |
| KCl | 0.149 | 0.149 g | 8.62 g |
| CaCl2 ⦁ 2H2O | 147 | 2 mL of 1 M CaCl2 stock | 250 µL of 1 M CaCl2 stock |
| HEPES | 238.3 | 1.19 g | 1.19 g |
| D-(+)-glucose | 180.2 | 0.541 g | 0. 541 g |
Table 1. Solutions for Dissection and Experimental Preparation. Displayed in this table are the recipes for artificial perilymph and artificial endolymph solutions used in dissection and in one- or two-chamber preparations. The solutions should be brought to pH 7.2 - 7.4 with about 2 mL of NaOH (perilymph) or 2 mL KOH (endolymph). The osmotic strength should read approximately 230 mmol·kg-1 due to incomplete ionic dissociation.