The American bullfrog's (Rana catesbeiana) sacculus permits direct examination of hair-cell physiology. Here the dissection and preparation of the bullfrog's sacculus for biophysical studies is described. We show representative experiments from these hair cells, including the calculation of a bundle's force-displacement relation and measurement of its unforced motion.
The study of hearing and balance rests upon insights drawn from biophysical studies of model systems. One such model, the sacculus of the American bullfrog, has become a mainstay of auditory and vestibular research. Studies of this organ have revealed how sensory cells hair can actively detect signals from the environment. Because of these studies, we now better understand the mechanical gating and localization of a hair cell's transduction channels, calcium's role in mechanical adaptation, and the identity of hair cell currents. This highly accessible organ continues to provide insight into the workings of hair cells. Here we describe the preparation of the bullfrog's sacculus for biophysical studies on its hair cells. We include the complete dissection procedure and provide specific protocols for the preparation of the sacculus in specific contexts. We additionally include representative results using this preparation, including the calculation of a hair bundle's instantaneous force-displacement relation and measurement of a bundle's spontaneous oscillation.
The acousticolateralis organs of mammals possess a complex architecture and lie within an anatomical niche that can be difficult to access. For example, the mammalian cochlea comprises a spiraling labyrinth and is embedded within the thick temporal bone. Isolation of the cochlea often causes mechanical damage to the sensory cells lying within it and has therefore proven to be a difficult task1. Neuroscientists have thus turned to model systems which are more readily extracted from the sanctum of the ear.
One of these model systems, the sacculus of the American bullfrog (Rana catesbeiana), has for decades yielded generalizable insight into the function of auditory and vestibular systems. The sacculus is a mixed-function organ with sensory roles in both low-frequency hearing and seismic sensation. The sensory cells of the sacculus are its hair cells, specialized transducers that convert mechanical energy into electrical signals within our auditory and vestibular organs. Projecting from the apical surface of each hair cell is a mechanosensitive hair bundle that comprises a graded tuft of enlarged microvilli called stereocilia. The tips of adjacent stereocilia are interconnected by filamentous tip-link proteins that mechanically gate ion channels in response to mechanical stimuli2,3. Although auditory and vestibular organs respond to different types of stimuli, they share a common detection mechanism. This commonality underlies the many insights gained into hair-cell mechanotransduction through studies of the bullfrog sacculus. For example, the hair cell's active process has been studied extensively in this organ4,5,6,7, and the hair bundle employs an energy-consuming process to produce mechanical work. Not only has it been shown that hair cells generate active work6, but distinct mechanisms underlying the active process and a hair cell's tuning characteristics have been unveiled through studies of bullfrog acousticolateralis organs. These include active hair-bundle motility8 and hair cell electrical resonance9,10,11 in the sacculus and frequency selectivity at the hair cell's ribbon synapse12 in the amphibian papilla.
The bullfrog's sacculus appeals to sensory neuroscientists for numerous reasons. Unlike the mammalian cochlea, this organ lies within the readily accessible otic capsule. Second, hair cells within this organ can remain healthy for several hours under appropriate conditions13,14. This permits experimentation on these cells over long timescales relative to their mammalian counterparts. Third, the organ bears little curvature, permitting easy manipulation. Fourth, each organ comprises a thousand or more hair cells15, providing both a high throughput and a high probability of locating an appropriate set of hair cells for a given experiment. Finally, the bullfrog's sacculus is easily visualized due to the thinness of this organ and large size of its hair cells.
These properties provide great versatility for the study of sensory cells within the bullfrog's sacculus. Depending on the question at hand, one of several experimental preparations can be obtained from the sacculus. The simplest of these is the one-chamber preparation. Here the sacculus is immobilized in a chamber filled with artificial perilymph, a sodium-rich and high-calcium saline. This preparation enables the study of hair cell currents and basic hair bundle mechanics. A second configuration, the two-chamber preparation, can be used to study spontaneous hair bundle movements. Here the apical side of hair cells is exposed to a potassium-rich and calcium-poor saline termed artificial endolymph, whereas the basolateral side is bathed in artificial perilymph. These two compartments mimic the in vivo arrangement of salines and provide an environment that allows hair bundles to oscillate spontaneously.
We describe in this paper the preparation of the bullfrog's sacculus for biophysical study of its sensory hair cells. We first provide a detailed depiction of the isolation of this organ from the frog's inner ear. We then describe both the one- and two-chamber experimental preparations and include representative results for each configuration.
Ethics Statement: All procedures were approved by the Institutional Animal Care and Use Committee (IACUC) at The Rockefeller University.
1. Pre-experimental Prespanparation
2. Experimental Tools
3. Extraction of Inner-ear Organs
4. One-chamber Preparation
5. Two-chamber Preparation
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.
Within the bullfrog's sacculus lie several thousand easily-accessible sensory hair cells. Here we demonstrate extraction and preparation of the sacculus for one- and two-chamber recordings. These two preparations permit both micromechanical and electrophysiological studies of hair cells and their associated bundles. Because the tissue can survive for several hours with frequent replacement of oxygenated saline, experiments may continue for long durations. Hair cells in these preparations typically remain viable for microelectrode recording for up to 6 h after dissection, while hair bundles oscillate spontaneously for up to 24 h after extraction.
Successful extraction and mounting of the sacculus hinges upon surmounting several common challenges. First, direct contact with the apical surface of the saccular macula should be avoided throughout the preparation procedure. The saccular nerve provides a convenient handle for safe manipulation of the sacculus. Once freed from the remainder of the inner-ear organs, the sacculus should be transferred using a large-bore pipette while remaining immersed in fluid to avoid mechanical damage to its sensory epithelium. The removal of otoconia from the macular surface must be completed without mechanical damage to hair cells. Because the otoconia lie directly atop the macula, hair cells can be damaged by accidental contact between dissection tools and the otolithic membrane while removing otoconia. To avoid damage, we recommend that the gelatinous mass of otoconia be held at a location far from the macula and removed as a single mass. This avoids fragmentation of the otoconial mass into numerous clusters, each of which would be individually extracted. If small clusters of otoconia remain they can be removed with gentle fluid pressure delivered by a Pasteur pipette. A final challenge involves the formation of a tight seal between the sacculus and aluminum mounting square in the two-chamber preparation. Employing a square with a perforation small enough to allow overlap of about 100 μm between the sacculus and the surrounding aluminum permits complete sealing of the tissue. The glue should be brought into contact with approximately 100 μm of saccular tissue around the macula's perimeter in order to form a tight seal.
The concentration of free Ca2+ is an important consideration in the study of hair cells. Ca2+ regulates both fast and slow adaptation, thus determining the kinetics of the mechanotransduction apparatus and the characteristics of the hair bundle's active-process phenomena, including spontaneous bundle motion8,23. Endolymphatic calcium in vivo is present at 250 μM, therefore the most physiologically relevant kinetics are assessed at this concentration (Maunsell J. H. R., R. Jacobs, and A. J. Hudspeth. Unpublished observations16). However, microelectrode recordings from hair cells require an external calcium concentration exceeding 2 mM for proper sealing of the cellular membrane around the microelectrode. It is therefore imperative to use a high-calcium saline for these experiments. Finally, one may wish to study the effects of external calcium upon mechanotransduction using a variety of calcium concentrations. In these cases, it is important to remember that calcium concentrations below 1 μM typically lead to tip-link rupture and irreversible loss of transduction28.
The two experimental preparations described here allow for a range of biophysical measurements on hair cells. However, additional measurements can be made with slight modifications to these preparations. In the folded saccular preparation, hair bundles are visualized laterally. Imaging hair-bundle motion from this vantage point reveals coherent motion of both short and tall stereocilia29. Here the saccular macula is first separated from its underlying tissue and subsequently folded along the axis defined by the saccular nerve such that hair bundles face outwards and are visualized laterally at the crease. A second modification, hair-cell dissociation, enables the study of both the hair cell's bundle and its soma. Hair cells are mechanically dissociated onto a glass slide for imaging and electrophysiological recording30. Finally, hair cells can be extruded from the epithelium by following a similar dissociation protocol but without the mechanical dissociation step. This treatment results in hair cells that gradually extrude out of the epithelium, providing basolateral access for electrophysiological recordings while minimizing mechanical damage. These preparations and their many modifications demonstrate the versatility of the frog sacculus as a model system for the biophysical study of sensory hair cells.
The authors have nothing to disclose.
The authors wish to acknowledge Dr. A. J. Hudspeth for funding and expertise in developing the preparations described in this paper. We also wish to thank Brian Fabella for creating and maintaining much of the custom equipment and software used in this protocol.
J. B. A. is supported by grant F30DC014215, J. D. S. is supported by grant F30DC013468, and both J. B. A. and J. D. S. are supported by grant T32GM07739 from the National Institutes of Health.
Common to both preparations | |||
Stereo-dissection microscope | Leica | MZ6 | Other sources can be used |
Tricaine methanesulfonate | Sigma | E10521 | Other sources can be used |
Metal pithing rod | Fine Science Tools | 10140-01 | |
Vannas spring scissors | Fine Science Tools | 15000-03 | |
Dumont #5 forceps | Fine Science Tools | 11252-20 | |
Glass Pasteur pipette and bulb (x2) | Fisher Scientific | 22-042816 | |
Fine eyelash mounted on a hypodermic needle | Fisher Scientific | 22-557-172 | |
Dow-corning vacuum grease | Fisher Scientific | 14-635-5C | |
Syringe for vacuum grease | Fisher Scientific | 14-829-45 | Other sources can be used |
35 mm Petri dish (x2-3) | Fisher Scientific | 08-772A | Other sources can be used |
Micropipette puller | Sutter | P-97 or P-2000 | |
120 V Solenoid puller | Home-made, see parts list | ||
Sputter coater | Anatech USA | Hummer 6.2 | |
Current source for iontophoresis | Axon Instruments | AxoClamp 2B | Other sources can be used |
Piezoelectric actuator | Piezosystem Jena | P-150-00 | |
Amplifier for piezoelectric actuator | Piezosystem Jena | ENV800 | |
Borosilicate glass capillary | World Precision Instruments | 1B120F-3 | |
Name | Company | Catalog Number | Comments |
For one-chamber preparation | |||
Microelectrode amplifier | Axon Instruments | AxoClamp 2B | Can be used for iontophoresis and microelectrode recordings simultaneously |
Magnetic pins (x2) | Home-made, see parts list | ||
Open-top chamber with magnetic sheet | Home-made, see parts list | ||
Name | Company | Catalog Number | Comments |
For two-chamber preparation | |||
Upper chamber | Supplementary file 1 | ||
Troughed lower chamber | Supplementary file 2 | ||
Aluminum foil | Fisher Scientific | 01-213-100 | Other sources can be used |
Mounting block | Supplementary file 3 | ||
Wooden applicator sticks | Fisher Scientific | 23-400-112 | Other sources can be used |
Teflon sheet | McMaster-Carr | 8545K12 | For teflon applicator |
Cyanoacrylate glue | 3M | 1469SB | |
Lab tissues (Kimwipes) | Fisher Scientific | 06-666A | Other sources can be used |
Gentamicin sulfate | Sigma-Aldrich | G1914 | Other sources can be used |
Quick-setting epoxy | McMaster-Carr | 7605A18 | |
18 mm glass coverslips | Fisher Scientific | 12-546 | Other sources can be used |
Name | Company | Catalog Number | Comments |
Saline components | |||
NaCl | Fisher Scientific | S271-3 | Other sources can be used |
KCl | Sigma-Aldrich | P4504-500G | Other sources can be used |
CaCl2 • 2H2O | Fisher Scientific | 10035-04-8 | Other sources can be used |
HEPES | Sigma-Aldrich | H3375-100G | Other sources can be used |
D-(+)-glucose | Sigma-Aldrich | G7021 | Other sources can be used |
Name | Company | Catalog Number | Comments/Description |
Parts lists for home-made equipment | |||
Solenoid puller | |||
Solenoid | Guardian Electric | A420-065426-00 | Other sources can be used |
Foot-pedal switch | Linemaster | T-51-SC36 | Other sources can be used |
Pipette holder | World Precision Instruments | MEH900R | Other sources can be used |
Coarse manipulator | Narishige Group | MM-3 | Other sources can be used |
Platinum wire | Alfa Aesar | 25093 | Other sources can be used |
Power supply | Leica | Z050-261 | Other sources can be used |
Name | Company | Catalog Number | Comments/Description |
Magnetic pins | |||
Epoxy | McMaster-Carr | 7556A33 | Other sources can be used |
1 mm thickness aluminum | McMaster-Carr | 89015K45 | Other sources can be used |
Insect pins | Fine Science Tools | 26000-40 | Other sources can be used |
Name | Company | Catalog Number | Comments/Description |
Open-top magnetic chamber | |||
Flexible magnetic strip | McMaster-Carr | 5759K75 | Other sources can be used |
1 mm thickness aluminum | McMaster-Carr | 89015K45 | Other sources can be used |