Changes in cochlear microphonic and neural sensitivity produced by acoustic trauma

Mechanical responses of the mammalian cochlea

Recent findings in auditory research have significantly changed our views of the processes involved in hearing. Novel techniques and new approaches to investigate the mammalian cochlea have expanded our knowledge about the mechanical events occurring at physiologically relevant stimulus intensities. Experiments performed in the apical, low-frequency regions demonstrate that although there is a change in the mechanical responses along the cochlea, the fundamental characteristics are similar across the frequency range. The mechanical responses to sound stimulation exhibit tuning properties comparable to those measured intracellularly or from nerve fibres. Non-linearities in the mechanical responses have now clearly been observed at all cochlear locations. The mechanics of the cochlea are vulnerable, and dramatic changes are seen especially when the sensory hair cells are affected, for example, following acoustic overstimulation or exposure to ototoxic compounds such as furosemide. The results suggest that there is a sharply tuned and vulnerable response related to the hair cells, superimposed on a more robust, broadly tuned response. Studies of the micromechanical behaviour down to the cellular level have demonstrated significant differences radially across the hearing organ and have provided new information on the important mechanical interactions with the tectorial membrane. There is now ample evidence of reverse transduction in the auditory periphery, i.e. the cochlea does not only receive and detect mechanical stimuli but can itself produce mechanical motion. Hence, it has been shown that electrical stimulation elicits motion within the cochlea very similar to that evoked by sound. In addition, the presence of acoustically-evoked displacements of the hearing organ have now been demonstrated by several laboratories.

Transient changes in cochlear potentials and DPOAEs after low-frequency tones: the 'two-minute bounce' revisited

After exposure to a loud, non-traumatic low-frequency tone, auditory thresholds are elevated. Thresholds recover to normal in a non-monotonic manner, decreasing rapidly at first before increasing again, until they finally decrease monotonically towards normal. Although the transient elevation of thresholds after the initial improvement was originally called a 'bounce' by Hirsh and Ward (1952), Kemp (1986) suggests that the initial rapid recovery is the oddity: under some conditions a low-frequency tone can produce hypersensitivity in otoacoustic emissions, psychophysical thresholds, and perceived loudness (Kemp's 'bounce') without a later elevation of threshold (Hirsh and Ward's 'bounce'). Kemp also suggested that the transient hypersensitivity was caused by changes in the sensitivity of the active process within the cochlea. We have investigated the origin of this transient hypersensitivity (Kemp's bounce) in guinea pigs, recording cochlear potentials (CM, CAP, SP and EP) and otoacoustic emissions (DPOAEs at f2-f1, 2f1-f2, 2f2-2f1 and 3f1-2f2). Our results indicate that the bounce does not require neural activity, but is probably produced by non-neural cochlear mechanisms, possibly a transient decrease in the permeability of the organ of Corti which produces a small but significant change in standing current through outer hair cells. At least part of these changes, which are reduced as the stimulation frequency increases, and absent above 2 kHz, seem due to a small and transient movement of the cochlear partition towards scala tympani, probably due to a transient osmotic imbalance.

Characterizing cochlear mechano-electric transduction in ears damaged with pure tones

Cochlear microphonics were recorded in response to Gaussian noise from the round window of Mongolian gerbils. A nonlinear systems identification procedure provided the frequency-domain parameters of a third-order polynomial equation describing cochlear mechano-electric transduction (MET). Exposure to an 8 kHz pure tone at 100 dB SPL for 20 min reduced the magnitude of the linear, quadratic, and cubic terms significantly. Animals exposed to a 1- or 4-kHz pure tone showed changes in the quadratic term. Differentiation of the polynomial equation and algebraic manipulations of the coefficients provided physiologic indices of MET. The sensitivity, saturation voltages, and sound pressures required to saturate MET were altered in animals exposed to an 8-kHz pure tone. Limited changes occurred in animals exposed to a 1- or 4-kHz pure tone.

Acoustic and electric forward-masking of the auditory nerve compound action potential: evidence for linearity of electro-mechanical transduction

We investigated electro-mechanical transduction within the cochlea by comparing masking of the auditory nerve compound action potential (CAP) by acoustical and electrical maskers. Forward-masking of the CAP reflects the response to the masker of the cochlear location tuned to the probe. Electrical stimulation was delivered through bipolar stimulating electrodes within the basal turn of the scala tympani. The growth of masking of high-frequency probes which excite cochlear locations close to the stimulating electrodes was similar for both acoustic and electrical maskers, suggesting a linear transduction of electrical energy to mechanical energy. Exposure to intense acoustic stimulation caused an equal loss of sensitivity to acoustic and electrical maskers. Masking of lower-frequency probes by electrical maskers increased rapidly with masker current, suggesting the direct electrical stimulation of neural elements. This masking was reduced by the administration of strychnine suggesting a contribution by the efferents towards masking of these low-frequency probes.

Regeneration of broken tip links and restoration of mechanical transduction in hair cells

A hair cell's tip links are thought to gate mechanoelectrical transduction channels. The susceptibility of tip links to acoustic trauma raises questions as to whether these fragile structures can be regenerated. We broke tip links with the calcium chelator 1,2-bis(O-aminophenoxy) ethane-N,N,N',N'-tetraacetic acid and found that they can regenerate, albeit imperfectly, over several hours. The time course of tip-link regeneration suggests that this process may underlie recovery from temporary threshold shifts induced by noise exposure. Cycloheximide does not block tip-link regeneration, indicating that new protein synthesis is not required. The calcium ionophore ionomycin prevents regeneration, suggesting regeneration normally may be stimulated by the reduction in stereociliary Ca2+ when gating springs rupture and transduction channels close. Supporting the equivalence of tip links with gating springs, mechanoelectrical transduction returns over the same time period as tip links; strikingly, adaptation is substantially reduced, even 24 hr after breaking tip links.

Selective inner hair cell loss does not alter distortion product otoacoustic emissions

Outer hair cells (OHC) are believed to be the dominant source of distortion product otoacoustic emissions (DPOAE) in mammals; however, some studies in genetic mutants suggest that inner hair cell (IHC) loss may lead to a significant reduction of DPOAE amplitude. In the present study, we determined the extent to which IHC loss altered DPOAE amplitude by using carboplatin to destroy selectively the IHCs in the chinchilla while sparing virtually all of the OHCs. IHC losses of 80-100% with normal retention of OHCs did not reduce the amplitude of the DPOAEs or the cochlear microphonic potential (CM); however, it completely abolished the compound action potential (CAP). The only time that the amplitude of the DPOAEs and CM were reduced was in cases where both the IHCs and OHCs were destroyed in the base of the cochlea. We conclude that the total loss of IHCs does not lead to a significant change in DPOAE amplitude. DPOAE amplitude was only reduced when there was a significant loss of OHCs.

Nonlinear feedback models for the tuning of auditory nerve fibers

The tuning of auditory nerve (AN) fibers is generally characterized by an increase in bandwidth and, for mid- to high-frequency fibers, a downward shift in the center frequency as sound level increases. Changes in bandwidth are accompanied by changes in the phase properties of the fibers; thus the timing of neural discharges also changes as a function of sound level. This study focuses on the magnitude and phase properties of models designed to reproduce the nonlinear properties of AN fibers that were studied electrophysiologically. The forward path of each model consisted of a linear second-order resonance, and each feedback path contained a saturating nonlinearity. In model 1, the feedback path was a simple memoryless, saturating nonlinearity. In model 2, a low-pass filter was added after the feedback nonlinearity. The ability of each model to simulate aspects of the nonlinear tuning of AN fibers is discussed. Model 2 was able to simulate a wider range of nonlinear behavior for different AN fibers and thus has promise for use in simulations of populations of fibers tuned to different frequencies.

Effects of kainic acid on the cochlear potentials and distortion product otoacoustic emissions in chinchilla

In absence of acoustic stimulation, the auditory nerve generates electrical noise with a spectral peak between 300 and 3000 Hz (Dolan et al., 1990). This electrical noise is eliminated when the dendrites of auditory nerve fibers are damaged by kainic acid (KA). We hypothesized that the KA-induced damage to the afferent dendrites might alter cochlear micromechanics or modify outer hair cell (OHC) electromotility. The KA-induced decrease in spontaneous electrical noise from the auditory nerve could conceivably reduce the spontaneous sounds recorded in the ear canal and the postulated change in cochlear micromechanics might alter distortion product otoacoustic emissions (DPOAE). To evaluate these hypotheses, we applied KA to the round window of the cochlea. KA reduced the spontaneous electrical noise recorded from the round window and significantly reduced the amplitude of the compound action potential (CAP) to tone bursts at 2, 4 and 8 kHz. KA caused only a slight reduction in the amplitude of the cochlear microphonic (CM) recorded from the round window: however, it had no effect on the spontaneous acoustic noise in the car canal or on 2 f1-f2 DPOAEs. These results suggest that the KA-induced reduction of electrical noise from the auditory nerve has no measurable effect on OHC electromotility as reflected in spontaneous otoacoustic emissions and that damage to the afferent dendrites has no effect on cochlear micromechanics as reflected in DPOAEs.

Effects of acoustic overstimulation on 2f1-f2 distortion product in the cochlear microphonics

The cochlear microphonics (CM) in response to two-tone stimuli as well as the threshold of compound action potential (CAP) were measured before and after exposure to 4 kHz pure tone at 100 dB SPL for 10 min. Although the loss of CM output at the primary frequencies was limited to around 2 dB, the 2f1-f2 distortion products in the CM (CM-DPs) were markedly reduced immediately after the exposure, especially at low primary levels (i.e. less than 65 dB). The low level CM-DPs recovered gradually near the initial level within 7 days from the exposure. The elevation of CAP threshold closely paralleled with the reduction of CM-DPs in not only the acute phase but also in the recovery phase from the exposure. These results show that the active transduction process in the cochlea was affected by acoustic overstimulation. This impairment of the active transduction was postulated to play an important role in developing the noise induced temporary threshold shift.

Spatiotemporal encoding of sound level: models for normal encoding and recruitment of loudness

This study explores the hypothesis that sound level is encoded in the spatiotemporal response patterns of auditory nerve (AN) fibers. The temporal properties of AN fiber responses depend upon sound level due to nonlinearities in the auditory periphery. In particular, the compressive nonlinearity of the inner ear introduces systematic changes in the timing of the responses of AN fibers as a function of level. Changes in single fiber responses that depend upon both sound level and characteristic frequency (CF) result in systematic changes in the spatiotemporal response patterns across populations of AN fibers. This study investigates the changes in the spatiotemporal response patterns as a function of level using a computational model for responses of low-frequency AN fibers. A mechanism that could extract information encoded in this form is coincidence detection across AN fibers of different CFs. This study shows that this mechanism could play a role in encoding of sound level for simple and complex stimuli. The model demonstrates that this encoding scheme would be influenced by auditory pathology that affects the peripheral compressive nonlinearity in a way that is consistent with the phenomenon of recruitment of loudness, which often accompanies sensorineural hearing loss.

Rapid changes in the frequency tuning of neurons in cat auditory cortex resulting from pure-tone-induced temporary threshold shift

The response areas (frequency by intensity) of single neurons in primary auditory cortex of anesthetized cats were studied before and after temporary threshold shifts in cochlear sensitivity induced by an intense pure tone. Cochlear temporary threshold shift was monitored through the threshold of the gross auditory nerve compound action potential and in most cases involved a notch-like loss centered at the characteristic frequency of the unit under study. Only two neurons showed changes in response area that mirrored the changes at the auditory periphery. Most neurons (14) showed more complex changes involving both expansion and contraction of response areas. Expansion of response areas was indicated by lower thresholds at some frequencies and by the emergence of sensitivity to previously ineffective frequencies. A change was classified as contraction when the response area after the intense-tone exposure was smaller than would be expected by applying the profile of the temporary threshold shift to the initial response area. Contraction of both upper (high intensity) and lower boundaries of response areas was found; in the most extreme cases, neurons were totally unresponsive after the intense-tone exposure. The complexity of effects of temporary threshold shifts on the response areas of cortical neurons is likely to be related to mechanisms that normally determine the frequency response limits of these neurons. The response areas of cortical neurons are more complex than those of auditory nerve fibers, and are thought to reflect the integration of excitatory and inhibitory inputs. The variety of effects observed in this study are consistent with the excitatory and inhibitory components of the response area of a given neuron being differentially affected by the temporary threshold shift.

Auditory degeneration after acoustic trauma in two genotypes of mice

Two strains of mice, CBA/Ca and C57BL/6J, were exposed to a steady noise (2-7 kHz) of 120 dB SPL for 5 min at 1, 3, 6, or 12 months of age. Threshold shifts were determined by recording auditory brainstem response 1 month after exposure and thereafter up to the age of 16 months (C57BL) or 23-27 months (CBA). With increasing age of exposure, susceptibility to acoustic trauma at middle frequencies (6.3-12.5 kHz) 1 month after exposure decreased in CBA mice but remained constant in C57BL mice. With increasing age after exposure, threshold shifts were retained at the middle frequencies in CBA mice exposed at 1 month of age and in C57BL mice of all exposed groups. The progress of the interaction between the previous noise damage and aging effects was generally the same for the two strains, first an additivity and then a blocking-like interaction. The rate of the progress in post-noise hearing did not exceed the spontaneous rate of aging. The differences between exposed and non-exposed groups decreased with advancing age. The results indicate that the interaction of noise trauma and aging effects depends on the susceptibility of the individual to acoustic trauma, affected frequencies, and the severity of noise-induced PTS. A previous noise damage did not potentiate the auditory degeneration either in CBA/Ca or in C57BL/6J mice.

Additivity of threshold elevations produced by disruption of outer hair cell function

We present a simple model describing the additivity of hearing loss in the mammalian cochlea produced by disruption of the outer hair cell transduction processes. The validity of this model has been tested experimentally in the guinea-pig by inducing threshold elevations using two simultaneous cochlear manipulations, including acoustic overstimulation, two-tone suppression, low-frequency acoustic biasing of the cochlear partition and electrical stimulation of the medial olivo-cochlear system of efferent fibres. The results of these experiments suggest that the model presented is an adequate description, within the measurement error of our experiments, of the hearing losses produced.

Cochlear efferent neurones and protection against acoustic trauma: protection of outer hair cell receptor current and interanimal variability

We have measured the changes in neural and microphonic sensitivity in the basal turn of the guinea-pig cochlea produced by intense acoustic overstimulation (10 kHz, 115 dB SPL for 60 s and 150 s). As reported previously, the drop in neural and microphonic sensitivities observed after overstimulation were highly correlated [Patuzzi et al. (1989) Hear. Res. 39, 189-202]. Presentation of a non-traumatizing pure-tone to the contralateral ear (10 kHz, 80 dB SPL) during acoustic overstimulation reduced the amount of acoustic trauma measured using the neural response or the microphonic response. Transection of the medial olivo-cochlear system of efferent fibres at the floor of the fourth ventricle abolished this protective effect of contralateral sound and dramatically reduced the variability in the data. Since the low-frequency microphonic is a simple measure of the receptor current through the outer hair cells, and this current probably plays a part in enhancing the mechanical sensitivity of the cochlea, the protection of the microphonic we have observed suggests that the efferent system protects neural sensitivity by protecting the mechano-electrical transduction of outer hair cells. The drop in variability after sectioning the efferents also suggests that inter-animal variations in susceptibility to noise trauma may be a consequence of differing tonic activity of the efferents, and/or a variation in the sensitivity of the efferent pathway.

Basilar membrane nonlinearity and its influence on auditory nerve rate-intensity functions

Previous papers have shown that the shapes of rate-intensity functions of auditory nerve fibres vary with spontaneous rate (Sachs and Abbas 1974; Sachs et al. 1989; Winter et al. 1990; Yates et al. 1990), and that the variation is due to the nonlinear properties of the basilar membrane. This paper examines the basilar membrane nonlinearity and provides a semi-quantitative explanation for it in terms of previous models (Zwicker 1979; Patuzzi et al. 1989) and an analogue model. It thereby provides explanations for the shapes of the basilar membrane input-output curves and for the way in which they vary with trauma. The shapes of the neural rate-intensity functions are quantified and shown to be consistent with the low-threshold data of Geisler et al. (1985). Several nonlinear properties of the cochlea, such as recruitment, are also interpreted.

The ototoxic mechanism of cisplatin

The ototoxic mechanism of cisplatin was investigated. Potentiation of cisplatin ototoxicity by furosemide and amino-oxyacetic acid (AOAA) was observed. Substantial hearing loss in cisplatin-deafened animals was accompanied by normal values of the endocochlear potential and a reduction in the sensitivity of the 2f1-f2 distortion products. The loss in dB of the sensitivity of the distortion products correlated extremely well with the loss of the neural sensitivity in dB. There was also a relationship between the fractional reduction of the low frequency (1000 Hz) microphonic potential and hearing loss in dB. Iontophoresis of cisplatin into scala media resulting in the immediate loss of neural thresholds at the site of iontophoresis. It is concluded that cisplatin caused the hearing loss by blocking OHC transduction channels.

Basilar membrane nonlinearity determines auditory nerve rate-intensity functions and cochlear dynamic range

In a previous paper (Winter et al., 1990) we demonstrated the existence of a new type of auditory-nerve rate-intensity function, the straight type, as well as a correlation between rate-level type, threshold and spontaneous rate. In this paper we now show that the variation in rate-intensity functions has its origin in the basilar membrane nonlinearity. Comparison of rate-intensity functions at characteristic frequency and at a tail-frequency show that the rate-intensity functions are identical at low firing rates and that the sloping-saturation and straight types deviate from the standard function only at higher firing rates. The frequencies at which the deviations occur, and the change from saturating to sloping-saturation or straight, are closely correlated with the characteristic frequency of the fibre. Using the tail-frequency rate-intensity function as a calibration, it is possible to derive the basilar membrane input-output function at characteristic frequency from the characteristic frequency rate-intensity function. The resulting derived basilar membrane input-output functions are of a simple form and agree well with published direct measurements of basilar membrane motion. They show that the wide dynamic range to which the cochlea responds, about 120 decibels, is compressed by the basilar membrane nonlinearity into a much smaller range of about 30-35 decibels. General characteristics of the derived basilar membrane input-output curves show features which agree well with psychoacoustic studies of loudness estimation.

Does electrical stimulation of the crossed olivo-cochlear bundle produce movement of the organ of Corti?

Low-frequency microphonic waveforms have been recorded in the basal turn of the guinea pig cochlea with and without electrical stimulation of the crossed olivocochlear bundle (COCB) at the floor of the fourth ventricle. Stimulation of the COCB increased the amplitude of the microphonic waveforms as described previously, but did not alter the shape of the waveforms markedly. The changes observed with COCB stimulation are consistent with a reduction in the impedance of the basolateral wall of the outer hair cells by about 50%, and possibly a 20% increase in the vibration of the organ of Corti at low frequencies, but suggest little or no change in the operating point on the transfer curve relating deflection of the hair bundles to the receptor current through the hair cells. It therefore seems that if slow contraction of the outer hair cells occurs during acute efferent stimulation in vivo, then it produces only a small deflection of the outer hair cell stereocilia, equivalent to a transverse displacement of the organ of Corti of less than 1.5 nm.

Saturation of outer hair cell receptor currents causes two-tone suppression

Zwicker [Biol. Cybern. 35, 243-250, (1979); J. Acoust. Soc. Am. 80, 163-176 (1986)] has previously proposed that many nonlinear phenomena in the mammalian cochlea can be explained by saturation of a positive feedback process which enhances mechanical sensitivity, although the site of the nonlinearity producing this saturation has so far remained obscure. In this paper we present evidence suggesting that the nonlinearity of mechano-electrical transduction in the outer hair cells is the dominant nonlinearity producing two-tone suppression in the mammalian cochlea. In particular, we show that: (i) suppression of the extracellular summating potential (SP), recorded from a particular place within the organ of Corti, has characteristics similar to the suppression of activity in the auditory-nerve; (ii) that SP suppression occurs at approximately constant basilar membrane displacement, inferred from the SP iso-response contours; and that (iii) the onset of SP suppression with suppressor tones on the tail of the frequency tuning curve closely parallels the onset of nonlinearity in the local cochlear microphonic. Since previous studies (Patuzzi et al., 1989) have demonstrated that the vibration of the basilar membrane at its characteristic frequency is very sensitive to changes in outer hair cell receptor current, we consider that interference in outer hair cell currents caused by nonlinearity in mechano-electrical transduction is an adequate explanation of two-tone suppression. This requires that outer hair cell receptor currents deviate from linearity at a suppressor tone level below that required to produce a significant DC receptor potential within the inner hair cells, and that the active process within the cochlea is distributed along a local region of the cochlea, basal of the vibration peak.

Outer hair cell receptor current and sensorineural hearing loss

It is argued in this paper that many nonlinear phenomena in audition and many types of sensorineural hearing loss can be explained by a disruption of the mechano-electrical transduction process at the apex of the outer hair cells. This is done using experimental data and a simple model of the active role of outer hair cells in cochlear mechanics based on our previous experiments with acoustic trauma. The causes of sensorineural loss addressed include acoustic trauma, aminoglycoside ototoxicity, intoxication with loop diuretics, hypoxia and Meniere's disease. The nonlinear phenomena discussed include loudness compression, two-tone suppression and modulation of cochlear sensitivity by very low-frequency tones. In every case considered the reduction in neural sensitivity was related to the reduction in outer hair cell receptor current in a quantitatively similar way. We conclude that the link is causal.

The origin of the low-frequency microphonic in the first cochlear turn of guinea-pig

Low-frequency microphonic potentials (100 Hz to 2000 Hz) have been measured in the first turn of the guinea pig cochlea before and after a variety of manipulations of the cochlea. These included ablation of the apical turns, iontophoresis of streptomycin, dc current injection into the first turn, acoustic trauma and two-tone interference with pure tones. These manipulations indicate that the low-frequency microphonic measured in the first turn and at the round window is generated predominantly by the hair cells of this region. It is a convenient and relatively uncomplicated indicator of the integrity of the mechano-electrical transduction process of these cells.