An Overview of Electrically Evoked Otoacoustic Emissions in the Mammalian Cochlea

AbstractAlternating currents injected into the cochlea are able to evoke outer hair cell-mediated basilar membrane motion, thus give rise to production of otoacoustic emissions. This electrically evoked otoacoustic emission(EEOAE) provides a useful tool for the research of out hair cell electromotility in vivo. This article reviews the research work on EEOAEs in mammals. Features of the EEOAEs and theories of their generation are introduced. Methods of EEOAE measurement are also described

Contribution of the anterior inferior cerebellar artery to cochlear blood flow in guinea pig: A model-based analysis

This study was performed to determine the contribution of the anterior inferior cerebellar artery (AICA) to cochlear blood flow (CBF) in guinea pig. The AICA and the basilar-vertebral arterial complex in twelve animals was exposed through the basal portion of the skull. The cochlea was ventrally approached and the CBF of the apical area monitored with laser Doppler flowmetry. A specially designed microclamp was held in a micromanipulator and used to obstruct the AICA. When the AICA was clamped, CBF decreased to approximately 60% of baseline (BL) (not to `biological zero'), followed by a gradual increase. When the clamp was released, CBF quickly increased to more than 160% BL and then slowly declined to baseline. To quantify the contribution of AICA to CBF, we formulated an electrical analog model of the cochlear vessel system. With this model, AICA contribution to CBF and the relationship among blood pressure, blood flow, and vascular resistance or vascular conductance in the cochlea can be explored. Results in the present study indicate that the AICA contributes only about 45% of CBF to the cochlea; 55% of CBF must come from other supplying vessels. Contrary to previous reports, CBF response to AICA clamping did not exhibit a stable or constant decrease but showed time-dependent dynamic changes. In addition, the cochlear vascular system showed a marked autoregulatory response, instead of a passive response, to the perfusion pressure change. AICA clamping is, therefore, not a suitable model for investigation of ischemia effects in the guinea pig cochlea, but it is a useful approach to study autoregulation and the myogenic mechanism of the cochlear vascular system.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/30403/1/0000023.pd

Successor Liability in Bankruptcy: Some Unifying Themes of Intertemporal Creditor Priorities Created by Running Covenants, Products Liability, and Toxic-Waste Cleanup

The exceptional sensitivity of mammalian hearing organs is attributed to an active process, where force produced by sensory cells boost sound-induced vibrations, making soft sounds audible. This process is thought to be local, with each section of the hearing organ capable of amplifying sound-evoked movement, and nearly instantaneous, since amplification can work for sounds at frequencies up to 100 kHz in some species. To test these fundamental precepts, we developed a method for focally stimulating the living hearing organ with light. Light pulses caused intense and highly damped mechanical responses followed by traveling waves that developed with considerable delay. The delayed response was identical to movements evoked by click-like sounds. This shows that the active process is neither local nor instantaneous, but requires mechanical waves traveling from the cochlear base toward its apex. A physiologically-based mathematical model shows that such waves engage the active process, enhancing hearing sensitivity.Funding Agencies|NIH [DC-004554, DC-004084]; Swedish Research Council [K2011-63X-14061-11-39]; Research Council for Health, Working Life and Welfare [2006-1526]; Horselskadades Riksforbund; Tysta skolan foundation</p

Розробка модуля Ethernet контролю для дистанційного керування електроживильною установкою

Sound processing in the inner ear involves separation of the constituent frequencies along the length of the cochlea. Frequencies relevant to human speech (100 to 500 Hz) are processed in the apex region. Among mammals, the guinea pig cochlear apex processes similar frequencies and is thus relevant for the study of speech processing in the cochlea. However, the requirement for extensive surgery has challenged the optical accessibility of this area to investigate cochlear processing of signals without significant intrusion. A simple method is developed to provide optical access to the guinea pig cochlear apex in two directions with minimal surgery. Furthermore, all prior vibration measurements in the guinea pig apex involved opening an observation hole in the otic capsule, which has been questioned on the basis of the resulting changes to cochlear hydrodynamics. Here, this limitation is overcome by measuring the vibrations through the unopened otic capsule using phase-sensitive Fourier domain optical coherence tomography. The optically and surgically advanced method described here lays the foundation to perform minimally invasive investigation of speech-related signal processing in the cochlea. (C) The Authors. Published by SPIE under a Creative Commons Attribution 3.0 Unported License.Funding Agencies|NIH NIDCD [R01DC000141]; NIH [R01DC004554, R01DC010201, R01DC011796]; Swedish Research Council [K2014-63X-14061-14-5]; Torsten Soderberg Foundation</p

Spontaneous Basilar Membrane Oscillation and Otoacoustic Emission at 15 kHz in a Guinea Pig

A spontaneous otoacoustic emission (SOAE) measured in the ear canal of a guinea pig was found to have a counterpart in spontaneous mechanical vibration of the basilar membrane (BM). A spontaneous 15-kHz BM velocity signal was measured from the 18-kHz tonotopic location and had a level close to that evoked by a 14-kHz, 15-dB SPL tone given to the ear. Lower-frequency pure-tone acoustic excitation was found to reduce the spontaneous BM oscillation (SBMO) while higher-frequency sound could entrain the SBMO. Octave-band noise centered near the emission frequency showed an increased narrow-band response in that frequency range. Applied pulses of current enhanced or suppressed the oscillation, depending on polarity of the current. The compound action potential (CAP) audiogram demonstrated a frequency-specific loss at 8 and 12 kHz in this animal. We conclude that a relatively high-frequency spontaneous oscillation of 15 kHz originated near the 15-kHz tonotopic place and appeared at the measured BM location as a mechanical oscillation. The oscillation gave rise to a SOAE in the ear canal. Electric current can modulate level and frequency of the otoacoustic emission in a pattern similar to that for the observed mechanical oscillation of the BM.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/41384/1/10162_2004_Article_4045.pd

Localization of the Cochlear Amplifier in Living Sensitive Ears

BACKGROUND: To detect soft sounds, the mammalian cochlea increases its sensitivity by amplifying incoming sounds up to one thousand times. Although the cochlear amplifier is thought to be a local cellular process at an area basal to the response peak on the spiral basilar membrane, its location has not been demonstrated experimentally. METHODOLOGY AND PRINCIPAL FINDINGS: Using a sensitive laser interferometer to measure sub-nanometer vibrations at two locations along the basilar membrane in sensitive gerbil cochleae, here we show that the cochlea can boost soft sound-induced vibrations as much as 50 dB/mm at an area proximal to the response peak on the basilar membrane. The observed amplification works maximally at low sound levels and at frequencies immediately below the peak-response frequency of the measured apical location. The amplification decreases more than 65 dB/mm as sound levels increases. CONCLUSIONS AND SIGNIFICANCE: We conclude that the cochlea amplifier resides at a small longitudinal region basal to the response peak in the sensitive cochlea. These data provides critical information for advancing our knowledge on cochlear mechanisms responsible for the remarkable hearing sensitivity, frequency selectivity and dynamic range

A mechanoelectrical mechanism for detection of sound envelopes in the hearing organ

To understand speech, the slowly varying outline, or envelope, of the acoustic stimulus is used to distinguish words. A small amount of information about the envelope is sufficient for speech recognition, but the mechanism used by the auditory system to extract the envelope is not known. Several different theories have been proposed, including envelope detection by auditory nerve dendrites as well as various mechanisms involving the sensory hair cells. We used recordings from human and animal inner ears to show that the dominant mechanism for envelope detection is distortion introduced by mechanoelectrical transduction channels. This electrical distortion, which is not apparent in the sound-evoked vibrations of the basilar membrane, tracks the envelope, excites the auditory nerve, and transmits information about the shape of the envelope to the brain.Funding Agencies|Swedish Research Council [K2014-63X-14061-14-5, 2017-06092]; Torsten Soderberg foundation; Strategic research area for systems neurobiology (Region Ostergotland); Linkoping University; NIH-NIDCD [R01 DC-004554, R01 DC 000141]</p

Polarized-Light Intravital Microscopy for Study of Cochlear Microcirculation

Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/30483/1/0000111.pd

Diagrams for measuring basilar membrane vibrations.

<p>(A) Two measured locations on the BM and one on the stapes (red dots). As the wave travels from the base to its BF location (B), the cochlear amplifier increases the BM vibration at a location basal to the BF site (blue bar in panel C). The local transfer function can specifically quantify the functioning of the amplification region between positions A and B. (D) shows a sharp peak at ∼15.3 kHz at low sound levels, which was >1,000 at 20 dB SPL. As the sound level increased, the peak magnitude decreased, and the peak broadened and shifted toward ∼12.0 kHz. (E and H) Growth rates in dB/dB at the more basal (E) and apical (H) locations. (F) The phase lag progressively increased with frequency. The data in panels G–I, measured at the more apical location, are similar to those in panels D–F (allowing for a lower BF). BM_B and BM_A are BM vibration magnitudes at the measured basal and apical locations.</p